2023
DOI: 10.1088/1751-8121/acd312
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Covariant definition of double null data and geometric uniqueness of the characteristic initial value problem

Abstract: The characteristic Cauchy problem of the Einstein field equations has been recently addressed from a completely abstract viewpoint by means of hypersurface data and, in particular, via the notion of double null data. However, this definition was given in a partially gauge-fixed form. In this paper we generalize the notion of double null data in a fully diffeomorphism and gauge covariant way, and show that the definition is complete by proving that no extra conditions are needed to embed the double null data in some… Show more

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Cited by 6 publications
(4 citation statements)
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“…We also establish the connection between the intrinsic and extrinsic (embedding) pictures. Similar results have been obtained by Mars, Sánchez-Pérez, and Manzano [81][82][83], who developed the intrinsic geometry of hypersurfaces of arbitrary causal type, referred to as the geometrical hypersurface data formalism. Additionally, we include the expressions for all components of the Einstein equation, the general symmetries of a stretched horizon beyond the tangential ones, and the corresponding Noether charges.…”
Section: Introductionsupporting
confidence: 81%
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“…We also establish the connection between the intrinsic and extrinsic (embedding) pictures. Similar results have been obtained by Mars, Sánchez-Pérez, and Manzano [81][82][83], who developed the intrinsic geometry of hypersurfaces of arbitrary causal type, referred to as the geometrical hypersurface data formalism. Additionally, we include the expressions for all components of the Einstein equation, the general symmetries of a stretched horizon beyond the tangential ones, and the corresponding Noether charges.…”
Section: Introductionsupporting
confidence: 81%
“…In Section 3, we consider a family of sCarrollian structures sC r = (v i (r), k j (r), h ij (r), ρ(r)) labeled by the function r. The stretched horizon with different r can now be considered the leaves of the r = constant foliation of the surrounding spacetime. By utilizing the Mars-Senovilla rigging technique [79,80] (see also [38,96] for situations involving null surfaces), we explicitly establish the correspondence between the two viewpoints and derive the relations between the sCarrollian structure and the rigging structure, including the sCarrollian connection and the sCarrollian stress tensor (see also [81][82][83]). We also discuss the arbitrariness in the embedding of the sCarrollian structure into the spacetime, leading to more general gauge fixings than those adopted in [1].…”
Section: Summary Of the Resultsmentioning
confidence: 99%
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“…The maximal globally hyperbolic solution is uniquely determined by the data, up to isometry. This can be seen by first noting that the local solution is defined uniquely, up to isometry, by the data listed; see [42] for an extensive discussion. Choosing a spacelike Cauchy hypersurface within the domain of existence of the coordinate solution, one can appeal to the usual Choquet-Bruhat-Geroch uniqueness theorem for the spacelike Cauchy problem to conclude.…”
Section: The Existence Theorem For Two Null Hypersurfaces Intersectin...mentioning
confidence: 99%